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module phystokenc_m |
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! $Header: /home/cvsroot/LMDZ4/libf/phylmd/phystokenc.F,v 1.2 2004/06/22 11:45:35 lmdzadmin Exp $ |
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! |
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c |
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c |
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SUBROUTINE phystokenc ( |
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I pdtphys,rlon,rlat, |
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I pt,pmfu, pmfd, pen_u, pde_u, pen_d, pde_d, |
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I pfm_therm,pentr_therm, |
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I pcoefh,yu1,yv1,ftsol,pctsrf, |
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I frac_impa,frac_nucl, |
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I pphis,paire,dtime,itap) |
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USE ioipsl |
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USE histcom |
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use dimens_m |
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use indicesol |
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use dimphy |
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use conf_gcm_m |
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use tracstoke |
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IMPLICIT none |
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c====================================================================== |
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c Auteur(s) FH |
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c Objet: Moniteur general des tendances traceurs |
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c |
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c====================================================================== |
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c====================================================================== |
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c Arguments: |
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c |
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c EN ENTREE: |
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c ========== |
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c |
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c divers: |
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c ------- |
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c |
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real pdtphys ! pas d'integration pour la physique (seconde) |
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c |
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integer physid, itap |
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save physid |
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integer ndex2d(iim*(jjm+1)),ndex3d(iim*(jjm+1)*klev) |
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c convection: |
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c ----------- |
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c |
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REAL pmfu(klon,klev) ! flux de masse dans le panache montant |
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REAL pmfd(klon,klev) ! flux de masse dans le panache descendant |
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REAL pen_u(klon,klev) ! flux entraine dans le panache montant |
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REAL pde_u(klon,klev) ! flux detraine dans le panache montant |
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REAL pen_d(klon,klev) ! flux entraine dans le panache descendant |
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REAL pde_d(klon,klev) ! flux detraine dans le panache descendant |
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real pt(klon,klev),t(klon,klev) |
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c |
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REAL, intent(in):: rlon(klon), rlat(klon) |
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real dtime |
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REAL zx_tmp_3d(iim,jjm+1,klev),zx_tmp_2d(iim,jjm+1) |
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c Couche limite: |
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c -------------- |
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c |
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REAL pcoefh(klon,klev) ! coeff melange CL |
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REAL yv1(klon) |
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REAL yu1(klon),pphis(klon),paire(klon) |
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c Les Thermiques : (Abderr 25 11 02) |
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c --------------- |
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REAL pfm_therm(klon,klev+1) |
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real fm_therm1(klon,klev) |
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REAL pentr_therm(klon,klev) |
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REAL entr_therm(klon,klev) |
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REAL fm_therm(klon,klev) |
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c |
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c Lessivage: |
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c ---------- |
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c |
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REAL frac_impa(klon,klev) |
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REAL frac_nucl(klon,klev) |
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c |
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c Arguments necessaires pour les sources et puits de traceur |
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C |
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real ftsol(klon,nbsrf) ! Temperature du sol (surf)(Kelvin) |
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real pctsrf(klon,nbsrf) ! Pourcentage de sol f(nature du sol) |
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c====================================================================== |
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c |
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INTEGER i, k |
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c |
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REAL mfu(klon,klev) ! flux de masse dans le panache montant |
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REAL mfd(klon,klev) ! flux de masse dans le panache descendant |
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REAL en_u(klon,klev) ! flux entraine dans le panache montant |
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REAL de_u(klon,klev) ! flux detraine dans le panache montant |
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REAL en_d(klon,klev) ! flux entraine dans le panache descendant |
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REAL de_d(klon,klev) ! flux detraine dans le panache descendant |
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REAL coefh(klon,klev) ! flux detraine dans le panache descendant |
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REAL pyu1(klon),pyv1(klon) |
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REAL pftsol(klon,nbsrf),ppsrf(klon,nbsrf) |
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real pftsol1(klon),pftsol2(klon),pftsol3(klon),pftsol4(klon) |
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real ppsrf1(klon),ppsrf2(klon),ppsrf3(klon),ppsrf4(klon) |
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REAL dtcum |
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integer iadvtr,irec |
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real zmin,zmax |
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logical ok_sync |
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save t,mfu,mfd,en_u,de_u,en_d,de_d,coefh,dtcum |
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save fm_therm,entr_therm |
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save iadvtr,irec |
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save pyu1,pyv1,pftsol,ppsrf |
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data iadvtr,irec/0,1/ |
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c |
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c Couche limite: |
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c====================================================================== |
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ok_sync = .true. |
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print*,'Dans phystokenc.F' |
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print*,'iadvtr= ',iadvtr |
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print*,'istphy= ',istphy |
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print*,'istdyn= ',istdyn |
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IF (iadvtr.eq.0) THEN |
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CALL initphysto('phystoke', |
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. rlon,rlat,dtime, dtime*istphy,dtime*istphy,nqmx,physid) |
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write(*,*) 'apres initphysto ds phystokenc' |
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ENDIF |
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c |
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ndex2d = 0 |
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ndex3d = 0 |
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i=itap |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1,pphis,zx_tmp_2d) |
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CALL histwrite(physid,"phis",i,zx_tmp_2d,iim*(jjm+1),ndex2d) |
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c |
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i=itap |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1,paire,zx_tmp_2d) |
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CALL histwrite(physid,"aire",i,zx_tmp_2d,iim*(jjm+1),ndex2d) |
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iadvtr=iadvtr+1 |
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c |
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if (mod(iadvtr,istphy).eq.1.or.istphy.eq.1) then |
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print*,'reinitialisation des champs cumules |
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s a iadvtr=',iadvtr |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=0. |
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mfd(i,k)=0. |
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en_u(i,k)=0. |
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de_u(i,k)=0. |
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en_d(i,k)=0. |
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de_d(i,k)=0. |
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coefh(i,k)=0. |
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t(i,k)=0. |
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fm_therm(i,k)=0. |
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entr_therm(i,k)=0. |
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enddo |
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enddo |
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do i=1,klon |
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pyv1(i)=0. |
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pyu1(i)=0. |
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end do |
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do k=1,nbsrf |
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do i=1,klon |
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pftsol(i,k)=0. |
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ppsrf(i,k)=0. |
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enddo |
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enddo |
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dtcum=0. |
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endif |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=mfu(i,k)+pmfu(i,k)*pdtphys |
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mfd(i,k)=mfd(i,k)+pmfd(i,k)*pdtphys |
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en_u(i,k)=en_u(i,k)+pen_u(i,k)*pdtphys |
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de_u(i,k)=de_u(i,k)+pde_u(i,k)*pdtphys |
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en_d(i,k)=en_d(i,k)+pen_d(i,k)*pdtphys |
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de_d(i,k)=de_d(i,k)+pde_d(i,k)*pdtphys |
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coefh(i,k)=coefh(i,k)+pcoefh(i,k)*pdtphys |
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t(i,k)=t(i,k)+pt(i,k)*pdtphys |
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fm_therm(i,k)=fm_therm(i,k)+pfm_therm(i,k)*pdtphys |
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entr_therm(i,k)=entr_therm(i,k)+pentr_therm(i,k)*pdtphys |
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enddo |
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enddo |
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do i=1,klon |
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pyv1(i)=pyv1(i)+yv1(i)*pdtphys |
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pyu1(i)=pyu1(i)+yu1(i)*pdtphys |
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end do |
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do k=1,nbsrf |
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do i=1,klon |
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pftsol(i,k)=pftsol(i,k)+ftsol(i,k)*pdtphys |
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ppsrf(i,k)=ppsrf(i,k)+pctsrf(i,k)*pdtphys |
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enddo |
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enddo |
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dtcum=dtcum+pdtphys |
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IF(mod(iadvtr,istphy).eq.0) THEN |
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c |
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c normalisation par le temps cumule |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=mfu(i,k)/dtcum |
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mfd(i,k)=mfd(i,k)/dtcum |
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en_u(i,k)=en_u(i,k)/dtcum |
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de_u(i,k)=de_u(i,k)/dtcum |
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en_d(i,k)=en_d(i,k)/dtcum |
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de_d(i,k)=de_d(i,k)/dtcum |
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coefh(i,k)=coefh(i,k)/dtcum |
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c Unitel a enlever |
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t(i,k)=t(i,k)/dtcum |
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fm_therm(i,k)=fm_therm(i,k)/dtcum |
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entr_therm(i,k)=entr_therm(i,k)/dtcum |
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enddo |
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enddo |
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do i=1,klon |
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pyv1(i)=pyv1(i)/dtcum |
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pyu1(i)=pyu1(i)/dtcum |
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end do |
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do k=1,nbsrf |
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do i=1,klon |
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pftsol(i,k)=pftsol(i,k)/dtcum |
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pftsol1(i) = pftsol(i,1) |
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pftsol2(i) = pftsol(i,2) |
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pftsol3(i) = pftsol(i,3) |
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pftsol4(i) = pftsol(i,4) |
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ppsrf(i,k)=ppsrf(i,k)/dtcum |
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ppsrf1(i) = ppsrf(i,1) |
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ppsrf2(i) = ppsrf(i,2) |
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ppsrf3(i) = ppsrf(i,3) |
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ppsrf4(i) = ppsrf(i,4) |
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enddo |
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enddo |
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c |
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c ecriture des champs |
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c |
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irec=irec+1 |
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ccccc |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, t, zx_tmp_3d) |
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CALL histwrite(physid,"t",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, mfu, zx_tmp_3d) |
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CALL histwrite(physid,"mfu",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, mfd, zx_tmp_3d) |
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CALL histwrite(physid,"mfd",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, en_u, zx_tmp_3d) |
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CALL histwrite(physid,"en_u",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, de_u, zx_tmp_3d) |
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CALL histwrite(physid,"de_u",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, en_d, zx_tmp_3d) |
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CALL histwrite(physid,"en_d",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, de_d, zx_tmp_3d) |
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CALL histwrite(physid,"de_d",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, coefh, zx_tmp_3d) |
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CALL histwrite(physid,"coefh",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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c ajou... |
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do k=1,klev |
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do i=1,klon |
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fm_therm1(i,k)=fm_therm(i,k) |
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enddo |
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enddo |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, fm_therm1, zx_tmp_3d) |
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CALL histwrite(physid,"fm_th",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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c |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1, entr_therm, zx_tmp_3d) |
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CALL histwrite(physid,"en_th",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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cccc |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1,frac_impa,zx_tmp_3d) |
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CALL histwrite(physid,"frac_impa",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(klev,klon,iim,jjm+1,frac_nucl,zx_tmp_3d) |
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CALL histwrite(physid,"frac_nucl",itap,zx_tmp_3d, |
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. iim*(jjm+1)*klev,ndex3d) |
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CALL gr_fi_ecrit(1, klon,iim,jjm+1, pyu1,zx_tmp_2d) |
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CALL histwrite(physid,"pyu1",itap,zx_tmp_2d,iim*(jjm+1), |
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. ndex2d) |
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CALL gr_fi_ecrit(1, klon,iim,jjm+1, pyv1,zx_tmp_2d) |
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CALL histwrite(physid,"pyv1",itap,zx_tmp_2d,iim*(jjm+1) |
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. ,ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, pftsol1, zx_tmp_2d) |
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CALL histwrite(physid,"ftsol1",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, pftsol2, zx_tmp_2d) |
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CALL histwrite(physid,"ftsol2",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, pftsol3, zx_tmp_2d) |
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CALL histwrite(physid,"ftsol3",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, pftsol4, zx_tmp_2d) |
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CALL histwrite(physid,"ftsol4",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf1, zx_tmp_2d) |
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CALL histwrite(physid,"psrf1",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf2, zx_tmp_2d) |
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CALL histwrite(physid,"psrf2",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf3, zx_tmp_2d) |
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CALL histwrite(physid,"psrf3",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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CALL gr_fi_ecrit(1,klon,iim,jjm+1, ppsrf4, zx_tmp_2d) |
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CALL histwrite(physid,"psrf4",itap,zx_tmp_2d, |
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. iim*(jjm+1),ndex2d) |
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if (ok_sync) call histsync(physid) |
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c if (ok_sync) call histsync |
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c |
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cAA Test sur la valeur des coefficients de lessivage |
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c |
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zmin=1e33 |
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zmax=-1e33 |
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do k=1,klev |
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do i=1,klon |
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zmax=max(zmax,frac_nucl(i,k)) |
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zmin=min(zmin,frac_nucl(i,k)) |
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enddo |
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enddo |
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Print*,'------ coefs de lessivage (min et max) --------' |
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Print*,'facteur de nucleation ',zmin,zmax |
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zmin=1e33 |
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zmax=-1e33 |
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do k=1,klev |
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do i=1,klon |
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zmax=max(zmax,frac_impa(i,k)) |
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zmin=min(zmin,frac_impa(i,k)) |
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enddo |
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enddo |
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Print*,'facteur d impaction ',zmin,zmax |
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ENDIF |
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c reinitialisation des champs cumules |
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go to 768 |
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if (mod(iadvtr,istphy).eq.1) then |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=0. |
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mfd(i,k)=0. |
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en_u(i,k)=0. |
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de_u(i,k)=0. |
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en_d(i,k)=0. |
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de_d(i,k)=0. |
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coefh(i,k)=0. |
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t(i,k)=0. |
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fm_therm(i,k)=0. |
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entr_therm(i,k)=0. |
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enddo |
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enddo |
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do i=1,klon |
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pyv1(i)=0. |
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pyu1(i)=0. |
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end do |
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do k=1,nbsrf |
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do i=1,klon |
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pftsol(i,k)=0. |
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ppsrf(i,k)=0. |
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enddo |
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enddo |
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dtcum=0. |
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endif |
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do k=1,klev |
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do i=1,klon |
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mfu(i,k)=mfu(i,k)+pmfu(i,k)*pdtphys |
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mfd(i,k)=mfd(i,k)+pmfd(i,k)*pdtphys |
|
|
en_u(i,k)=en_u(i,k)+pen_u(i,k)*pdtphys |
|
|
de_u(i,k)=de_u(i,k)+pde_u(i,k)*pdtphys |
|
|
en_d(i,k)=en_d(i,k)+pen_d(i,k)*pdtphys |
|
|
de_d(i,k)=de_d(i,k)+pde_d(i,k)*pdtphys |
|
|
coefh(i,k)=coefh(i,k)+pcoefh(i,k)*pdtphys |
|
|
t(i,k)=t(i,k)+pt(i,k)*pdtphys |
|
|
fm_therm(i,k)=fm_therm(i,k)+pfm_therm(i,k)*pdtphys |
|
|
entr_therm(i,k)=entr_therm(i,k)+pentr_therm(i,k)*pdtphys |
|
|
enddo |
|
|
enddo |
|
|
do i=1,klon |
|
|
pyv1(i)=pyv1(i)+yv1(i)*pdtphys |
|
|
pyu1(i)=pyu1(i)+yu1(i)*pdtphys |
|
|
end do |
|
|
do k=1,nbsrf |
|
|
do i=1,klon |
|
|
pftsol(i,k)=pftsol(i,k)+ftsol(i,k)*pdtphys |
|
|
ppsrf(i,k)=ppsrf(i,k)+pctsrf(i,k)*pdtphys |
|
|
enddo |
|
|
enddo |
|
2 |
|
|
3 |
dtcum=dtcum+pdtphys |
IMPLICIT NONE |
|
768 continue |
|
4 |
|
|
5 |
RETURN |
contains |
6 |
END |
|
7 |
|
SUBROUTINE phystokenc(pdtphys, pt, pmfu, pmfd, pen_u, pde_u, pen_d, pde_d, & |
8 |
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pfm_therm, pentr_therm, pcoefh, yu1, yv1, ftsol, pctsrf, frac_impa, & |
9 |
|
frac_nucl, pphis, paire, dtime) |
10 |
|
|
11 |
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! From phylmd/phystokenc.F, version 1.2 2004/06/22 11:45:35 |
12 |
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! Author: Fr\'ed\'eric Hourdin |
13 |
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! Objet : \'ecriture des variables pour transport offline |
14 |
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|
15 |
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use gr_phy_write_m, only: gr_phy_write |
16 |
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USE histwrite_m, ONLY: histwrite |
17 |
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USE histsync_m, ONLY: histsync |
18 |
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USE indicesol, ONLY: nbsrf |
19 |
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use initphysto_m, only: initphysto |
20 |
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USE dimphy, ONLY: klev, klon |
21 |
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use time_phylmdz, only: itap |
22 |
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USE tracstoke, ONLY: istphy |
23 |
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|
24 |
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REAL, INTENT (IN):: pdtphys ! pas d'integration pour la physique (seconde) |
25 |
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REAL, intent(in):: pt(klon, klev) |
26 |
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|
27 |
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! convection: |
28 |
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|
29 |
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REAL, INTENT (IN):: pmfu(klon, klev) ! flux de masse dans le panache montant |
30 |
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|
31 |
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REAL, intent(in):: pmfd(klon, klev) |
32 |
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! flux de masse dans le panache descendant |
33 |
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|
34 |
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REAL, intent(in):: pen_u(klon, klev) ! flux entraine dans le panache montant |
35 |
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REAL, intent(in):: pde_u(klon, klev) ! flux detraine dans le panache montant |
36 |
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|
37 |
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REAL, intent(in):: pen_d(klon, klev) |
38 |
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! flux entraine dans le panache descendant |
39 |
|
|
40 |
|
REAL, intent(in):: pde_d(klon, klev) |
41 |
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! flux detraine dans le panache descendant |
42 |
|
|
43 |
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! Les Thermiques |
44 |
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REAL, intent(in):: pfm_therm(klon, klev+1) |
45 |
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REAL, intent(in):: pentr_therm(klon, klev) |
46 |
|
|
47 |
|
! Couche limite: |
48 |
|
REAL, intent(in):: pcoefh(klon, klev) ! coeff melange Couche limite |
49 |
|
REAL, intent(in):: yu1(klon) |
50 |
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REAL, intent(in):: yv1(klon) |
51 |
|
|
52 |
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! Arguments necessaires pour les sources et puits de traceur |
53 |
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|
54 |
|
REAL, intent(in):: ftsol(klon, nbsrf) ! Temperature du sol (surf)(Kelvin) |
55 |
|
REAL, intent(in):: pctsrf(klon, nbsrf) ! Pourcentage de sol f(nature du sol) |
56 |
|
|
57 |
|
! Coefficients de lessivage: |
58 |
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REAL, intent(in):: frac_impa(klon, klev) ! facteur d'impaction |
59 |
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REAL, intent(in):: frac_nucl(klon, klev) ! facteur de nucleation |
60 |
|
|
61 |
|
REAL, INTENT(IN):: pphis(klon) |
62 |
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real, intent(in):: paire(klon) |
63 |
|
REAL, INTENT (IN):: dtime |
64 |
|
|
65 |
|
! Local: |
66 |
|
|
67 |
|
real t(klon, klev) |
68 |
|
INTEGER, SAVE:: physid |
69 |
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|
70 |
|
! Les Thermiques |
71 |
|
|
72 |
|
REAL fm_therm1(klon, klev) |
73 |
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REAL entr_therm(klon, klev) |
74 |
|
REAL fm_therm(klon, klev) |
75 |
|
|
76 |
|
INTEGER i, k |
77 |
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|
78 |
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REAL, save:: mfu(klon, klev) ! flux de masse dans le panache montant |
79 |
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REAL mfd(klon, klev) ! flux de masse dans le panache descendant |
80 |
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REAL en_u(klon, klev) ! flux entraine dans le panache montant |
81 |
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REAL de_u(klon, klev) ! flux detraine dans le panache montant |
82 |
|
REAL en_d(klon, klev) ! flux entraine dans le panache descendant |
83 |
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REAL de_d(klon, klev) ! flux detraine dans le panache descendant |
84 |
|
REAL coefh(klon, klev) ! flux detraine dans le panache descendant |
85 |
|
|
86 |
|
REAL pyu1(klon), pyv1(klon) |
87 |
|
REAL pftsol(klon, nbsrf), ppsrf(klon, nbsrf) |
88 |
|
REAL pftsol1(klon), pftsol2(klon), pftsol3(klon), pftsol4(klon) |
89 |
|
REAL ppsrf1(klon), ppsrf2(klon), ppsrf3(klon), ppsrf4(klon) |
90 |
|
|
91 |
|
REAL dtcum |
92 |
|
|
93 |
|
INTEGER:: iadvtr = 0, irec = 1 |
94 |
|
|
95 |
|
SAVE t, mfd, en_u, de_u, en_d, de_d, coefh, dtcum |
96 |
|
SAVE fm_therm, entr_therm |
97 |
|
SAVE pyu1, pyv1, pftsol, ppsrf |
98 |
|
|
99 |
|
!------------------------------------------------------ |
100 |
|
|
101 |
|
! Couche limite: |
102 |
|
|
103 |
|
IF (iadvtr==0) CALL initphysto('phystoke', dtime, dtime * istphy, & |
104 |
|
dtime * istphy, physid) |
105 |
|
|
106 |
|
CALL histwrite(physid, 'phis', itap, gr_phy_write(pphis)) |
107 |
|
CALL histwrite(physid, 'aire', itap, gr_phy_write(paire)) |
108 |
|
iadvtr = iadvtr + 1 |
109 |
|
|
110 |
|
IF (mod(iadvtr, istphy) == 1 .OR. istphy == 1) THEN |
111 |
|
PRINT *, 'reinitialisation des champs cumules a iadvtr =', iadvtr |
112 |
|
DO k = 1, klev |
113 |
|
DO i = 1, klon |
114 |
|
mfu(i, k) = 0. |
115 |
|
mfd(i, k) = 0. |
116 |
|
en_u(i, k) = 0. |
117 |
|
de_u(i, k) = 0. |
118 |
|
en_d(i, k) = 0. |
119 |
|
de_d(i, k) = 0. |
120 |
|
coefh(i, k) = 0. |
121 |
|
t(i, k) = 0. |
122 |
|
fm_therm(i, k) = 0. |
123 |
|
entr_therm(i, k) = 0. |
124 |
|
END DO |
125 |
|
END DO |
126 |
|
DO i = 1, klon |
127 |
|
pyv1(i) = 0. |
128 |
|
pyu1(i) = 0. |
129 |
|
END DO |
130 |
|
DO k = 1, nbsrf |
131 |
|
DO i = 1, klon |
132 |
|
pftsol(i, k) = 0. |
133 |
|
ppsrf(i, k) = 0. |
134 |
|
END DO |
135 |
|
END DO |
136 |
|
|
137 |
|
dtcum = 0. |
138 |
|
END IF |
139 |
|
|
140 |
|
DO k = 1, klev |
141 |
|
DO i = 1, klon |
142 |
|
mfu(i, k) = mfu(i, k) + pmfu(i, k) * pdtphys |
143 |
|
mfd(i, k) = mfd(i, k) + pmfd(i, k) * pdtphys |
144 |
|
en_u(i, k) = en_u(i, k) + pen_u(i, k) * pdtphys |
145 |
|
de_u(i, k) = de_u(i, k) + pde_u(i, k) * pdtphys |
146 |
|
en_d(i, k) = en_d(i, k) + pen_d(i, k) * pdtphys |
147 |
|
de_d(i, k) = de_d(i, k) + pde_d(i, k) * pdtphys |
148 |
|
coefh(i, k) = coefh(i, k) + pcoefh(i, k) * pdtphys |
149 |
|
t(i, k) = t(i, k) + pt(i, k) * pdtphys |
150 |
|
fm_therm(i, k) = fm_therm(i, k) + pfm_therm(i, k) * pdtphys |
151 |
|
entr_therm(i, k) = entr_therm(i, k) + pentr_therm(i, k) * pdtphys |
152 |
|
END DO |
153 |
|
END DO |
154 |
|
DO i = 1, klon |
155 |
|
pyv1(i) = pyv1(i) + yv1(i) * pdtphys |
156 |
|
pyu1(i) = pyu1(i) + yu1(i) * pdtphys |
157 |
|
END DO |
158 |
|
DO k = 1, nbsrf |
159 |
|
DO i = 1, klon |
160 |
|
pftsol(i, k) = pftsol(i, k) + ftsol(i, k) * pdtphys |
161 |
|
ppsrf(i, k) = ppsrf(i, k) + pctsrf(i, k) * pdtphys |
162 |
|
END DO |
163 |
|
END DO |
164 |
|
|
165 |
|
dtcum = dtcum + pdtphys |
166 |
|
|
167 |
|
IF (mod(iadvtr, istphy) == 0) THEN |
168 |
|
! normalisation par le temps cumule |
169 |
|
DO k = 1, klev |
170 |
|
DO i = 1, klon |
171 |
|
mfu(i, k) = mfu(i, k)/dtcum |
172 |
|
mfd(i, k) = mfd(i, k)/dtcum |
173 |
|
en_u(i, k) = en_u(i, k)/dtcum |
174 |
|
de_u(i, k) = de_u(i, k)/dtcum |
175 |
|
en_d(i, k) = en_d(i, k)/dtcum |
176 |
|
de_d(i, k) = de_d(i, k)/dtcum |
177 |
|
coefh(i, k) = coefh(i, k)/dtcum |
178 |
|
t(i, k) = t(i, k)/dtcum |
179 |
|
fm_therm(i, k) = fm_therm(i, k)/dtcum |
180 |
|
entr_therm(i, k) = entr_therm(i, k)/dtcum |
181 |
|
END DO |
182 |
|
END DO |
183 |
|
DO i = 1, klon |
184 |
|
pyv1(i) = pyv1(i)/dtcum |
185 |
|
pyu1(i) = pyu1(i)/dtcum |
186 |
|
END DO |
187 |
|
DO k = 1, nbsrf |
188 |
|
DO i = 1, klon |
189 |
|
pftsol(i, k) = pftsol(i, k)/dtcum |
190 |
|
pftsol1(i) = pftsol(i, 1) |
191 |
|
pftsol2(i) = pftsol(i, 2) |
192 |
|
pftsol3(i) = pftsol(i, 3) |
193 |
|
pftsol4(i) = pftsol(i, 4) |
194 |
|
|
195 |
|
ppsrf(i, k) = ppsrf(i, k)/dtcum |
196 |
|
ppsrf1(i) = ppsrf(i, 1) |
197 |
|
ppsrf2(i) = ppsrf(i, 2) |
198 |
|
ppsrf3(i) = ppsrf(i, 3) |
199 |
|
ppsrf4(i) = ppsrf(i, 4) |
200 |
|
END DO |
201 |
|
END DO |
202 |
|
|
203 |
|
! \'Ecriture des champs |
204 |
|
|
205 |
|
irec = irec + 1 |
206 |
|
|
207 |
|
CALL histwrite(physid, 't', itap, gr_phy_write(t)) |
208 |
|
CALL histwrite(physid, 'mfu', itap, gr_phy_write(mfu)) |
209 |
|
CALL histwrite(physid, 'mfd', itap, gr_phy_write(mfd)) |
210 |
|
CALL histwrite(physid, 'en_u', itap, gr_phy_write(en_u)) |
211 |
|
CALL histwrite(physid, 'de_u', itap, gr_phy_write(de_u)) |
212 |
|
CALL histwrite(physid, 'en_d', itap, gr_phy_write(en_d)) |
213 |
|
CALL histwrite(physid, 'de_d', itap, gr_phy_write(de_d)) |
214 |
|
CALL histwrite(physid, 'coefh', itap, gr_phy_write(coefh)) |
215 |
|
DO k = 1, klev |
216 |
|
DO i = 1, klon |
217 |
|
fm_therm1(i, k) = fm_therm(i, k) |
218 |
|
END DO |
219 |
|
END DO |
220 |
|
|
221 |
|
CALL histwrite(physid, 'fm_th', itap, gr_phy_write(fm_therm1)) |
222 |
|
CALL histwrite(physid, 'en_th', itap, gr_phy_write(entr_therm)) |
223 |
|
CALL histwrite(physid, 'frac_impa', itap, gr_phy_write(frac_impa)) |
224 |
|
CALL histwrite(physid, 'frac_nucl', itap, gr_phy_write(frac_nucl)) |
225 |
|
CALL histwrite(physid, 'pyu1', itap, gr_phy_write(pyu1)) |
226 |
|
CALL histwrite(physid, 'pyv1', itap, gr_phy_write(pyv1)) |
227 |
|
CALL histwrite(physid, 'ftsol1', itap, gr_phy_write(pftsol1)) |
228 |
|
CALL histwrite(physid, 'ftsol2', itap, gr_phy_write(pftsol2)) |
229 |
|
CALL histwrite(physid, 'ftsol3', itap, gr_phy_write(pftsol3)) |
230 |
|
CALL histwrite(physid, 'ftsol4', itap, gr_phy_write(pftsol4)) |
231 |
|
CALL histwrite(physid, 'psrf1', itap, gr_phy_write(ppsrf1)) |
232 |
|
CALL histwrite(physid, 'psrf2', itap, gr_phy_write(ppsrf2)) |
233 |
|
CALL histwrite(physid, 'psrf3', itap, gr_phy_write(ppsrf3)) |
234 |
|
CALL histwrite(physid, 'psrf4', itap, gr_phy_write(ppsrf4)) |
235 |
|
|
236 |
|
CALL histsync(physid) |
237 |
|
END IF |
238 |
|
|
239 |
|
END SUBROUTINE phystokenc |
240 |
|
|
241 |
|
end module phystokenc_m |